Undergrad Integration being unchanged after rotation

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The discussion centers on the invariance of an integral's value when the integration contour is rotated in the complex plane, specifically from the real axis to the imaginary axis. This is valid as long as the contour does not cross any poles of the integrand and the integrand approaches zero sufficiently quickly at infinity. The residue theorem supports this, stating that the integral of an entire function over a closed path is zero if there are no poles inside. By decomposing the original integral into the new rotated integral and two closed paths, the contributions from the closed paths vanish as their radius approaches infinity. Thus, the value of the integral remains unchanged after the contour rotation.
AndrewGRQTF
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This question is about the general 1 loop correction to the propagator in QFT (this is actually not important for this question). Let's say we have an integral over an integration variable x, and this x ranges from ##-\infty## to ##\infty##. If we look at this integration contour in the complex plane, it will be along the real axis. A book that I am reading (QFT by Srednicki), says that we can rotate this contour counterclockwise onto the imaginary axis, without changing the value of the integral, and he says that this is because the contour does not pass over any poles of the integrand and that the integrand vanishes fast enough as the magnitude of x goes to infinity.

My question is: why does the value of the integral not change when we change the integration contour?
 
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The integral of an entire function over a closed path is zero if there are no poles inside (residue theorem). If the function goes to zero sufficiently fast for large |z| you can write the original integral as sum of the new (rotated) integral plus two closed paths (two 90 degree sectors of the complex plane https://www.researchgate.net/figure/Integration-contour-in-the-complex-s-plane-to-compute-the-integral-representing-the_fig3_242423238, then let their radius go to infinity), the contribution from the closed paths is zero.
 
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mfb said:
The integral of an entire function over a closed path is zero if there are no poles inside (residue theorem). If the function goes to zero sufficiently fast for large |z| you can write the original integral as sum of the new (rotated) integral plus two closed paths (two 90 degree sectors of the complex plane https://www.researchgate.net/figure/Integration-contour-in-the-complex-s-plane-to-compute-the-integral-representing-the_fig3_242423238, then let their radius go to infinity), the contribution from the closed paths is zero.

Thank you.
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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